By Jan Roskam
A useful encyclopedia of historic airplane info, layout equations and methods.
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Extra resources for Airplane Design Parts I-VII
1 shows the most common transmission lines and guiding structures employed at RF and microwaves. On the one side, except for the circular dielectric waveguide where the EM field is confined by the dielectric discontinuity, we have conventional closed structures such as the coaxial cable and metal waveguides of various shapes, where the field is confined by metal walls. On the other side, we have planar, printed or integrated circuits fabricated on top of a thin dielectric substrate, such as the stripline or the microstrip line; because of their advantages in terms of reduced size, weight and cost, they are the most frequently employed transmission lines, except when the requirements of low loss or high power can only be matched by the use of waveguides.
We put B ¼ r Â A. 187) is preferred here as it yields dual expressions for E and H. 38 MICROWAVE AND RF ENGINEERING It is now the turn of the E field to be solenoidal. 197) become homogeneous. 199). Bibliography 1. 2. 3. 4. J. A. Stratton, Electromagnetic Theory, McGraw-Hill, New York, 1941. J. D. , New York, 1962. R. E. Collin, Foundations for Microwave Engineering, McGraw-Hill, New York, 1992. C. A. , New York, 1989. 1 Introduction Transmission lines are fundamental components of any RF apparatus or system.
16). The electric energy dissipates in the medium and is transformed into heat by the Joule effect. 32). We therefore have, for the average electric and magnetic energies stored in one period, 1 We ¼ Re 4 1 Wm ¼ Re 4 ! ð E Á D dV ¼ ð ð2:67Þ ! ð m H Á B* dV ¼ H Á H* dV 4 V V ð2:68Þ V ð e0 4 E Á E* dV * V while the time-averaged power dissipated is 1 Pd ¼ Re 2 ð ! ð s E Á J* dV ¼ E Á E* dV 2 V V ð2:69Þ the last equality holding for ohmic currents. s. s. 71) is the flow of the complex Poynting vector defined as 1 P ¼ E Â H* 2 entering into the volume V.
Airplane Design Parts I-VII by Jan Roskam